26 research outputs found
On the Accuracy of Calculated Reduction Potentials of Selected Group 8 (Fe, Ru, and Os) Octahedral Complexes
The
theoretical calculations of reduction potentials for the [MÂ(H<sub>2</sub>O)<sub>6</sub>]<sup>2+/3+</sup>, [MÂ(NH<sub>3</sub>)<sub>6</sub>]<sup>2+/3+</sup>, [MÂ(<i>en</i>)<sub>3</sub>]<sup>2+/3+</sup>, [MÂ(<i>bipy</i>)<sub>3</sub>]<sup>2+/3+</sup>, [MÂ(CN)<sub>6</sub>]<sup>4â/3â</sup>, and [MCl<sub>6</sub>]<sup>4â/3â</sup> systems (M = Fe, Os, Ru) were carried out.
The DFTÂ(PBE)/def2-TZVP//DFTÂ(PBE)/def2-SVP quantum chemical method
was employed to obtain presumably accurate ionization energies, whereas
the conductor-like screening model for real solvents (COSMO-RS) was
selected as the most suitable method for calculations of solvation
energies of the oxidized and reduced forms of the studied species.
It has been shown that COSMO-RS may overcome problems related to directionality
of hydrogen bonds in the second solvation sphere that previously led
to errors of âź1 V for the [RuÂ(H<sub>2</sub>O)<sub>6</sub>]<sup>2+</sup> complex employing PCM-like models. Thus, most of the values
for (2+) â (3+) oxidations are now within 0.1â0.2 V
from the experimental data, once the anticipated spinâorbit
coupling effects in Os complexes (downshifting the calculated reduction
potentials by âź0.3 V) are taken into account. The robustness
of the DFTÂ(PBE)/COSMO-RS computational protocol is further verified
by showing that reduction potentials obtained for selected 2+/3+ redox
pairs with and without the inclusion of explicit second-sphere water
molecules are almost identical. At the same time, it must be admitted
that the calculated values of reduction potentials for systems involving
quadruple charged species, exemplified here by [MÂ(CN)<sub>6</sub>]<sup>4â/3â</sup> and [MCl<sub>6</sub>]<sup>4â/3â</sup> redox pairs, might still not be within the grasp of contemporary
solvation models, possibly due to the large values of solvation energies
of their reduced (4â) forms that are in the range of 700â750
kcal mol<sup>â1</sup> (30â33 eV) and possibly larger
errors inherent in their calculations. Finally, a comparison is made
with M06-L//SMD computational protocol, which is also shown to correct
some of the deficiencies of previous PCM models
Predicting the Stability Constants of Metal-Ion Complexes from First Principles
The
most important experimental quantity describing the thermodynamics
of metal-ion binding with various (in)Âorganic ligands, or biomolecules,
is the stability constant of the complex (β). In principle,
it can be calculated as the free-energy change associated with the
metal-ion complexation, i.e., its uptake from the solution under standard
conditions. Because this process is associated with the interactions
of charged species, large values of interaction and solvation energies
are in general involved. Using the standard thermodynamic cycle (in
vacuo complexation and solvation/desolvation of the reference state
and of the resulting complexes), one usually subtracts values of several
hundreds of kilocalories per mole to obtain final results on the order
of units or tens of kilocalories per mole. In this work, we use density
functional theory and MøllerâPlesset second-order perturbation
theory calculations together with the conductor-like screening model
for realistic solvation to calculate the stability constants of selected
complexesî¸[MÂ(NH<sub>3</sub>)<sub>4</sub>]<sup>2+</sup>, [MÂ(NH<sub>3</sub>)<sub>4</sub>(H<sub>2</sub>O)<sub>2</sub>]<sup>2+</sup>, [MÂ(Imi)Â(H<sub>2</sub>O)<sub>5</sub>]<sup>2+</sup>, [MÂ(H<sub>2</sub>O)<sub>3</sub>(His)]<sup>+</sup>, [MÂ(H<sub>2</sub>O)<sub>4</sub>(Cys)], [MÂ(H<sub>2</sub>O)<sub>3</sub>(Cys)], [MÂ(CH<sub>3</sub>COO)Â(H<sub>2</sub>O)<sub>3</sub>]<sup>+</sup>, [MÂ(CH<sub>3</sub>COO)Â(H<sub>2</sub>O)<sub>5</sub>]<sup>+</sup>, [MÂ(SCH<sub>2</sub>COO)<sub>2</sub>]<sup>2â</sup>î¸with eight divalent metal ions (Mn<sup>2+</sup>, Fe<sup>2+</sup>, Co<sup>2+</sup>, Ni<sup>2+</sup>, Cu<sup>2+</sup>, Zn<sup>2+</sup>, Cd<sup>2+</sup>, and Hg<sup>2+</sup>). Using the currently available
computational protocols, we show that it is possible to achieve a <i>relative</i> accuracy of 2â4 kcal¡mol<sup>â1</sup> (1â3 orders of magnitude in β). However, because most
of the computed values are affected by metal- and ligand-dependent
systematic shifts, the accuracy of the âabsoluteâ (uncorrected)
values is generally lower. For metal-dependent systematic shifts,
we propose the specific values to be used for the given metal ion
and current protocol. At the same time, we argue that ligand-dependent
shifts (which cannot be easily removed) do not influence the metal-ion
selectivity of the particular site, and therefore it can be computed
to within 2 kcal¡mol<sup>â1</sup> average accuracy. Finally,
a critical discussion is presented that aims at potential caveats
that one may encounter in theoretical predictions of the stability
constants and highlights the perspective that theoretical calculations
may become both competitive and complementary tools to experimental
measurements
Predicting the Stability Constants of Metal-Ion Complexes from First Principles
The
most important experimental quantity describing the thermodynamics
of metal-ion binding with various (in)Âorganic ligands, or biomolecules,
is the stability constant of the complex (β). In principle,
it can be calculated as the free-energy change associated with the
metal-ion complexation, i.e., its uptake from the solution under standard
conditions. Because this process is associated with the interactions
of charged species, large values of interaction and solvation energies
are in general involved. Using the standard thermodynamic cycle (in
vacuo complexation and solvation/desolvation of the reference state
and of the resulting complexes), one usually subtracts values of several
hundreds of kilocalories per mole to obtain final results on the order
of units or tens of kilocalories per mole. In this work, we use density
functional theory and MøllerâPlesset second-order perturbation
theory calculations together with the conductor-like screening model
for realistic solvation to calculate the stability constants of selected
complexesî¸[MÂ(NH<sub>3</sub>)<sub>4</sub>]<sup>2+</sup>, [MÂ(NH<sub>3</sub>)<sub>4</sub>(H<sub>2</sub>O)<sub>2</sub>]<sup>2+</sup>, [MÂ(Imi)Â(H<sub>2</sub>O)<sub>5</sub>]<sup>2+</sup>, [MÂ(H<sub>2</sub>O)<sub>3</sub>(His)]<sup>+</sup>, [MÂ(H<sub>2</sub>O)<sub>4</sub>(Cys)], [MÂ(H<sub>2</sub>O)<sub>3</sub>(Cys)], [MÂ(CH<sub>3</sub>COO)Â(H<sub>2</sub>O)<sub>3</sub>]<sup>+</sup>, [MÂ(CH<sub>3</sub>COO)Â(H<sub>2</sub>O)<sub>5</sub>]<sup>+</sup>, [MÂ(SCH<sub>2</sub>COO)<sub>2</sub>]<sup>2â</sup>î¸with eight divalent metal ions (Mn<sup>2+</sup>, Fe<sup>2+</sup>, Co<sup>2+</sup>, Ni<sup>2+</sup>, Cu<sup>2+</sup>, Zn<sup>2+</sup>, Cd<sup>2+</sup>, and Hg<sup>2+</sup>). Using the currently available
computational protocols, we show that it is possible to achieve a <i>relative</i> accuracy of 2â4 kcal¡mol<sup>â1</sup> (1â3 orders of magnitude in β). However, because most
of the computed values are affected by metal- and ligand-dependent
systematic shifts, the accuracy of the âabsoluteâ (uncorrected)
values is generally lower. For metal-dependent systematic shifts,
we propose the specific values to be used for the given metal ion
and current protocol. At the same time, we argue that ligand-dependent
shifts (which cannot be easily removed) do not influence the metal-ion
selectivity of the particular site, and therefore it can be computed
to within 2 kcal¡mol<sup>â1</sup> average accuracy. Finally,
a critical discussion is presented that aims at potential caveats
that one may encounter in theoretical predictions of the stability
constants and highlights the perspective that theoretical calculations
may become both competitive and complementary tools to experimental
measurements
Accurate Prediction of One-Electron Reduction Potentials in Aqueous Solution by Variable-Temperature HâAtom Addition/Abstraction Methodology
A robust
and efficient theoretical approach for calculation of
the reduction potentials of charged species in aqueous solution is
presented. Within this approach, the reduction potential of a charged
complex (with a charge |<i>n|</i> ⼠2) is probed
by means of the reduction potential of its neutralized (protonated/deprotonated)
cognate, employing one or several H-atom addition/abstraction thermodynamic
cycles. This includes a separation of one-electron reduction from
protonation/deprotonation through the temperature dependence. The
accuracy of the method has been assessed for the set of 15 transition-metal
complexes that are considered as highly challenging systems for computational
electrochemistry. Unlike the standard computational protocol(s), the
presented approach yields results that are in excellent agreement
with experimental electrochemical data. Last but not least, the applicability
and limitations of the approach are thoroughly discussed
Reduction Pathways of 2,4,6-Trinitrotoluene: An Electrochemical and Theoretical Study
The reduction pathways of trinitrotoluene are studied
using electrochemical
and computational methods. The electrochemical reduction of three
nitro groups in 2,4,6-trinitrotoluene (TNT) is characterized by three
major reduction peaks in cyclic voltammograms at the peak potentials
of â0.310,
â0.463, and â0.629 V vs a normal hydrogen electrode
(NHE). The second and third peaks coincide
with the two peaks observed for the 2-amino-4,6-dinitrotoluene (at
the potentials of â0.475 and â0.627 V vs NHE), whereas
the two peaks in the 4-amino-2,6-dinitrotoluene voltammograms
appear at â0.537 and â0.623 V and deviate more significantly
from the corresponding two peaks
in 2,4,6-trinitrotoluene. It suggests that the first NO<sub>2</sub> group reduced in the overall process is the one in <i>ortho</i> position with respect to the CH<sub>3</sub> group. Analogously,
the 2,6-diamino-4-nitrotoluene exhibits a reduction peak at â0.629
V, almost identical to the third and second reduction peaks of 2,4,6-trinitrotoluene
and 2-amino-4,6-dinitrotoluene, respectively. Since the other isomer,
2,4-diamino-6-nitrotoluene, exhibits a reduction peak at â0.712
V, we conclude that the second reduction occurs also in the <i>ortho</i> position with respect to the methyl group. Most of
these observations are corroborated by quantum chemical calculations,
which yielded reduction potentials in a good agreement with the experimental
values (in relative scale). Thus, studying in detail all of the possible
protonation and redox states in the reduction of the first nitro group
and the key steps in the reduction of the second and third nitro groups,
we have obtained a comprehensive and detailed picture of the mechanism
of the full 18<i>e</i><sup>â</sup>/18H<sup>+</sup> reduction of TNT. Last but not least, the
calculations have shown that the thermodynamic stabilities of (isomeric)
neutral radical species (<b>X </b>+<b> </b><i><b>e</b></i><sup><b>â</b></sup><b> </b>+<b> H</b><sup><b>+</b></sup>)î¸presumably the regioselectivity-determining
steps
in the 6<i>e</i><sup>â</sup>/6H<sup>+</sup> reductions
of the individual NO<sub>2</sub> groupsî¸are within 2 kJ¡mol<sup>â1</sup> (i.e., comparable to RT). Therefore, the course of
the reduction
can be governed by the effect of the surroundings, such as the enzymatic
environment, and a different regioselectivity can be observed under
biological conditions
Computational Electrochemistry as a Reliable Probe of Experimentally Elusive Mononuclear Nonheme Iron Species
Despite the growing
number of reported Fe<sup>IV</sup>O complexes,
an unambiguous experimental characterization of their redox properties,
such as one-electron reduction potentials, remains a challenging task.
To this aim, we describe an efficient and straightforward theoretical
protocol for accurate calculations of redox potentials and calibrate
the protocol on a set of diverse 37 mononuclear nonheme iron (NHFe)
redox couples. It is shown that the methodology, further applied to
a set of 10 Fe<sup>IV</sup>O species, not only serves for near-quantitative
predictions of reduction potentials, but also is an elegant tool for
interpretation of the experimental electrochemical data. The general
need for such a computational methodology is illustrated on the prototypical
example of the (N4Py)ÂFe<sup>IV</sup>O complex, whose electrochemistry
has been studied for many years and still raises many questions
Accurate Prediction of One-Electron Reduction Potentials in Aqueous Solution by Variable-Temperature HâAtom Addition/Abstraction Methodology
A robust
and efficient theoretical approach for calculation of
the reduction potentials of charged species in aqueous solution is
presented. Within this approach, the reduction potential of a charged
complex (with a charge |<i>n|</i> ⼠2) is probed
by means of the reduction potential of its neutralized (protonated/deprotonated)
cognate, employing one or several H-atom addition/abstraction thermodynamic
cycles. This includes a separation of one-electron reduction from
protonation/deprotonation through the temperature dependence. The
accuracy of the method has been assessed for the set of 15 transition-metal
complexes that are considered as highly challenging systems for computational
electrochemistry. Unlike the standard computational protocol(s), the
presented approach yields results that are in excellent agreement
with experimental electrochemical data. Last but not least, the applicability
and limitations of the approach are thoroughly discussed
Computational Electrochemistry as a Reliable Probe of Experimentally Elusive Mononuclear Nonheme Iron Species
Despite the growing
number of reported Fe<sup>IV</sup>O complexes,
an unambiguous experimental characterization of their redox properties,
such as one-electron reduction potentials, remains a challenging task.
To this aim, we describe an efficient and straightforward theoretical
protocol for accurate calculations of redox potentials and calibrate
the protocol on a set of diverse 37 mononuclear nonheme iron (NHFe)
redox couples. It is shown that the methodology, further applied to
a set of 10 Fe<sup>IV</sup>O species, not only serves for near-quantitative
predictions of reduction potentials, but also is an elegant tool for
interpretation of the experimental electrochemical data. The general
need for such a computational methodology is illustrated on the prototypical
example of the (N4Py)ÂFe<sup>IV</sup>O complex, whose electrochemistry
has been studied for many years and still raises many questions
Reduction Pathways of 2,4,6-Trinitrotoluene: An Electrochemical and Theoretical Study
The reduction pathways of trinitrotoluene are studied
using electrochemical
and computational methods. The electrochemical reduction of three
nitro groups in 2,4,6-trinitrotoluene (TNT) is characterized by three
major reduction peaks in cyclic voltammograms at the peak potentials
of â0.310,
â0.463, and â0.629 V vs a normal hydrogen electrode
(NHE). The second and third peaks coincide
with the two peaks observed for the 2-amino-4,6-dinitrotoluene (at
the potentials of â0.475 and â0.627 V vs NHE), whereas
the two peaks in the 4-amino-2,6-dinitrotoluene voltammograms
appear at â0.537 and â0.623 V and deviate more significantly
from the corresponding two peaks
in 2,4,6-trinitrotoluene. It suggests that the first NO<sub>2</sub> group reduced in the overall process is the one in <i>ortho</i> position with respect to the CH<sub>3</sub> group. Analogously,
the 2,6-diamino-4-nitrotoluene exhibits a reduction peak at â0.629
V, almost identical to the third and second reduction peaks of 2,4,6-trinitrotoluene
and 2-amino-4,6-dinitrotoluene, respectively. Since the other isomer,
2,4-diamino-6-nitrotoluene, exhibits a reduction peak at â0.712
V, we conclude that the second reduction occurs also in the <i>ortho</i> position with respect to the methyl group. Most of
these observations are corroborated by quantum chemical calculations,
which yielded reduction potentials in a good agreement with the experimental
values (in relative scale). Thus, studying in detail all of the possible
protonation and redox states in the reduction of the first nitro group
and the key steps in the reduction of the second and third nitro groups,
we have obtained a comprehensive and detailed picture of the mechanism
of the full 18<i>e</i><sup>â</sup>/18H<sup>+</sup> reduction of TNT. Last but not least, the
calculations have shown that the thermodynamic stabilities of (isomeric)
neutral radical species (<b>X </b>+<b> </b><i><b>e</b></i><sup><b>â</b></sup><b> </b>+<b> H</b><sup><b>+</b></sup>)î¸presumably the regioselectivity-determining
steps
in the 6<i>e</i><sup>â</sup>/6H<sup>+</sup> reductions
of the individual NO<sub>2</sub> groupsî¸are within 2 kJ¡mol<sup>â1</sup> (i.e., comparable to RT). Therefore, the course of
the reduction
can be governed by the effect of the surroundings, such as the enzymatic
environment, and a different regioselectivity can be observed under
biological conditions
Macrocycle Conformational Sampling by DFT-D3/COSMO-RS Methodology
To
find and calibrate a robust and reliable computational protocol
for mapping conformational space of medium-sized molecules, exhaustive
conformational sampling has been carried out for a series of seven <i>macrocyclic</i> compounds of varying ring size and one acyclic
analogue. While five of them were taken from the MD/LLMOD/force field
study by Shelley and co-workers (Watts, K. S.; Dalal, P.; Tebben, A. J.; Cheney, D. L.; Shelley, J. C. Macrocycle Conformational Sampling with MacroModel. J. Chem. Inf. Model. 2014, 54, 2680â2696), three represent potential macrocyclic inhibitors of human cyclophilin
A. The free energy values (<i>G</i><sub>DFT/COSMOâRS</sub>) for all of the conformers of each compound were obtained by a composite
protocol based on <i>in vacuo</i> quantum mechanics (DFT-D3
method in a large basis set), standard gas-phase thermodynamics, and
the COSMO-RS solvation model. The <i>G</i><sub>DFT/COSMOâRS</sub> values were used as the reference for evaluating the performance
of conformational sampling algorithms: standard and extended MD/LLMOD
search (simulated-annealing molecular dynamics with low-lying eigenvector
following algorithms, employing the OPLS2005 force field plus GBSA
solvation) available in MacroModel and plain molecular dynamics (MD)
sampling at high temperature (1000 K) using the semiempirical quantum
mechanics (SQM) potential SQMÂ(PM6-D3H4/COSMO) followed by energy minimization
of the snapshots. It has been shown that the former protocol (MD/LLMOD)
may provide a more complete set of initial structures that ultimately
leads to the identification of a greater number of low-energy conformers
(as assessed by <i>G</i><sub>DFT/COSMOâRS</sub>)
than the latter (i.e., plain SQM MD). The CPU time needed to fully
evaluate one medium-sized <i>compound</i> (âź100 atoms,
typically resulting in several hundred or a few thousand conformers
generated and treated quantum-mechanically) is approximately 1,000â100,000
CPU hours on todayâs computers, which transforms to 1â7
days on a small-sized computer cluster with a few hundred CPUs. Finally,
our data sets based on the rigorous quantum-chemical approach allow
us to formulate a composite conformational sampling protocol with
multiple checkpoints and truncation of redundant structural data that
offers superior insights at affordable computational cost